13.07.2015 Views

Asymmetric fluid-structure dynamics in nanoscale imprint lithography

Asymmetric fluid-structure dynamics in nanoscale imprint lithography

Asymmetric fluid-structure dynamics in nanoscale imprint lithography

SHOW MORE
SHOW LESS
  • No tags were found...

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

length between the clamped-clamped ends of the actuator s<strong>in</strong>ce this length willvary when the actuators push and pull.ALFigure 5.3 Model of actuator for stiffness computationBeam bend<strong>in</strong>g equations approximate the stiffness of the distributedflexure r<strong>in</strong>g for each actuation arm. Each one-third segment of the distributedflexure can be modeled as a fixed-fixed beam as shown <strong>in</strong> Figure 5.4. Equation5.4 describes the bend<strong>in</strong>g of a fixed-fixed beam under a vertical load.FLbhFigure 5.4 Fixed-fixed beamF192EIδz= kδzL=3[5.4]3bhwhere I = . The flexure r<strong>in</strong>g is mach<strong>in</strong>ed from 7075-T6 alum<strong>in</strong>um alloy12with a Young’s modulus, E, of 72Gpa. The median radial length of the flexurer<strong>in</strong>g is 3.5 <strong>in</strong>ches. The flexure r<strong>in</strong>g is 1 <strong>in</strong>ch wide and 50 mils thick. With a total63

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!